EMCD

From Wikipedia, the free encyclopedia
Jump to: navigation, search

Electron magnetic circular dichroism (EMCD) (also known as Electron energy-loss Magnetic Chiral Dichroism) is the EELS[1] equivalent of XMCD.

The effect was first proposed in 2003[2] and experimentally confirmed in 2006[3] by the group of Prof. Peter Schattschneider at the Vienna University of Technology.

Similarly to XMCD, EMCD is a difference spectrum of two EELS spectra taken in a magnetic field with opposite helicities. Under appropriate scattering conditions[4] virtual photons with specific circular polarizations can be absorbed, giving rise to spectral differences. The largest difference is expected between the case where one virtual photon with left circular polarization and one with right circular polarization are absorbed. By closely analyzing the difference in the EMCD spectrum, information can be obtained on the magnetic properties of the atom, such as its spin and orbital magnetic moment.[5]

In the case of transition metals such as iron, cobalt, and nickel, the absorption spectra for EMCD are usually measured at the L-edge. This corresponds to the excitation of a 2p electron to a 3d state by the absorption of a virtual photon providing the ionisation energy. The absorption is visible as a spectral feature in the electron energy loss spectrum (EELS). Because the 3d electron states are the origin of the magnetic properties of the elements, the spectra contain information on the magnetic properties. Moreover, since the energy of each transition depends on the atomic number, the information obtained is element specific, that is, it is possible to distinguish the magnetic properties of a given element by examining the EMCD spectrum at its characteristic energy (708 eV for iron).

Since in both EMCD and XMCD the same electronic transitions are probed, the information obtained is the same. However EMCD has a higher spatial resolution[6][7] and depth sensitivity than its X-ray counterpart. Moreover EMCD can be measured on any TEM equipped with an EELS detector, whereas XMCD is normally measured only on dedicated synchrotron beamlines.

It has been recently demonstrated that electron vortex beams can be also used to measure EMCD.[8]

References[edit]

  1. ^ R F Egerton "Electron energy-loss spectroscopy in the TEM" Rep. Prog. Phys. 72 (2009) 016502
  2. ^ Hèbert, C and Schattschneider, P (2003). "A proposal for dichroic experiments in the electron microscope". Ultramicroscopy 96: 463–468. doi:10.1016/S0304-3991(03)00108-6. 
  3. ^ Schattschneider, P and Rubino, S and Hébert, C and Rusz, J and Kunes, J and Novak, P and Carlino, E and Fabrizioli, M and Panaccione, G. and Rossi, G (2006). "Detection of magnetic circular dichroism using a transmission electron microscope". Nature 441: 486–488. Bibcode:2006Natur.441..486S. doi:10.1038/nature04778. 
  4. ^ Hèbert, C and Schattschneider, P and Rubino, S and Novak, P and Rusz, J and Stöger-Pollach, M (2008). "Magnetic circular dichroism in Electron Energy Loss Spectrometry". Ultramicroscopy 108: 277–284. doi:10.1016/j.ultramic.2007.07.011. 
  5. ^ Rusz, J and Eriksson, O and Novak, P and Oppeneer, P M (2007). "Sum-rules for electron energy-loss near-edge spectra". Phys. Rev. B 76: 060408. arXiv:0706.0402. Bibcode:2007PhRvB..76f0408R. doi:10.1103/PhysRevB.76.060408. 
  6. ^ Schattschneider, P and Stöger-Pollach, M and Rubino, S and Sperl, M and Hurm, C and Zweck, J and Rusz, J (2008). "Detection of Magnetic Circular Dichroism on the 2 nm scale". Phys. Rev. B 78: 104413. Bibcode:2008PhRvB..78j4413S. doi:10.1103/PhysRevB.78.104413. 
  7. ^ Schattschneider, P and Hèbert, C and Rubino, S and Stöger-Pollach, M and Rusz, J and Novak, P (2008). "Magnetic circular dichroism in EELS: towards 10 nm resolution". Ultramicroscopy 108: 433–438. doi:10.1016/j.ultramic.2007.07.002. 
  8. ^ Verbeeck, J and Tian, H and Schattschneider, P (2010). "Production and application of electron vortex beams". Nature 467: 301–304. Bibcode:2010Natur.467..301V. doi:10.1038/nature09366. 

See also[edit]